Multi-mode temperature compensated filters and a method of constructing and compensating therefor

• US 5,589,807 A
• Filed: 06/07/1995
• Issued: 12/31/1996
• Est. Priority Date: 07/07/1994
• Status: Expired due to Fees

• Current Assignee: Com Dev Limited (Honeywell International Inc.)
• Original Assignee: Com Dev Limited (Honeywell International Inc.)
• Inventors: Tang, Wai-Cheung
• Primary Examiner(s): Lee, Benny
• Assistant Examiner(s): Bettendorf, Justin P.
• Application Number:
  US08/475,656
• Time in Patent Office: 573 Days
• Field of Search: 333/202, 333/212, 333/219.1, 333/227-232, 333/234, 333/235
• US Class Current: 333/212
• CPC Class Codes: H01P 1/2082 with multimode resonators H01P1/2086 takes precedence

Abstract

Multi-mode waveguide filters are temperature compensated using dielectric material contained within at least one cavity of a filter. The variation in operating frequency of the filter that would otherwise result from changes in temperature is substantially balanced by a change in operating frequency with temperature caused by a change in a dielectric constant of the dielectric material so that the operating frequency of the filter remains substantially constant with temperature. The filter can have one or more dual-mode or triple-mode cavities. In a method of constructing and compensating a filter, the amount of dielectric material is selected so that the dielectric material does not resonate at the operating frequency of the cavity, the amount of dielectric material in the cavity being adjustable after each cavity is constructed. The cavity is operated with a fixed amount of dielectric material contained in the cavity for each mode and the change in operating frequency of the filter with temperature is determined. If the change in operating frequency of the filter is not at an acceptable level, the amount of dielectric material contained in the cavity for each mode is varied and the filter is operated through a range of temperatures to determine whether the change in operating frequency is then at an acceptable level. These steps are repeated until the change in operating frequency of the filter is at an acceptable level.

Claims

1. A microwave filter comprising an input and output and a first cavity made of a material having a coefficient of thermal expansion and resonating at an operating frequency in at least two orthogonal modes substantially simultaneously, said cavity having a volume that is changeable with temperature, said cavity containing solid dielectric material having a dielectric constant that varies with temperature, said dielectric material being sized so that it does not resonate at the operating frequency of the cavity, there being at least one amount of said dielectric material having a value of a temperature coefficient of the dielectric constant to compensate for changes in the volume of the cavity with temperature to at least reduce a variation in said operating frequency that would otherwise by caused by a temperature-induced volume change of said cavity.

2. A filter as claimed in claim 1 wherein there are two amounts of dielectric material, one amount to primarily compensate for one mode and another amount to primarily compensate for another mode.

3. A filter as claimed in claim 2 wherein each amount of dielectric material is sized and located so that said operating frequency remains substantially constant as said temperature changes.

4. A filter as claimed in any one of claims 1, 2 or 3 wherein the volume of said first cavity increases as temperature increases and the dielectric constant of the dielectric material decreases as temperature increases.

5. A filter as claimed in any one of claims 1 or 2 wherein each amount of dielectric material is sized and located so that a change in said operating frequency of said filter is minimized.

6. A filter as claimed in claim 1 wherein said dielectric material is located at a maximum E-field location for at least one mode.

7. A filter as claimed in any one of claims 2 or 3 wherein one amount of dielectric material is located at a maximum E-field location for one mode and the other amount of dielectric material is located at a maximum E-field location for the other mode.

8. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric material is mounted on an adjustable susceptance such that the amount of dielectric material within the first cavity can be varied externally.

9. A filter as claimed in any one of claims 1, 2 or 3 wherein each amount of dielectric material is mounted on a screw that penetrates a wall of said first cavity so that the amount of dielectric material within said first cavity can be varied externally.

10. A filter as claimed in any one of claims 1, 2 or 3 wherein the dielectric material is mounted in a self-locking screw that penetrates a wall of said first cavity so that the amount of dielectric material within the cavity can be varied externally.

11. A filter as claimed in any one of claims 1, 2 or 3 wherein said first cavity has at least one tuning screw to tune at least one of the modes.

12. A filter as claimed in any one of claims 1, 2 or 3 wherein said first cavity has a coupling screw to couple energy between said modes.

13. A filter as claimed in any one of claims 1, 2 or 3 wherein said first cavity has a square or rectangular cross-section and resonates in two TE_10n modes, where n is a positive integer.

14. A filter as claimed in any one of claims 1, 2 or 3 wherein said first cavity has a circular cross-section and resonates in two TE_11n modes, where n is a positive integer.

15. A filter as claimed in any one of claims 1, 2 or 3 wherein the filter has a second cavity and said second cavity contains dielectric material having a temperature coefficient of the dielectric constant to compensate for changes in temperature, there being means to couple energy between said first cavity and said second cavity.

16. A filter as claimed in any one of claims 1, 2 or 3 wherein the amount of dielectric material is relatively small compared to the size of the cavity.

17. A filter as claimed in any one of claims 1, 2 or 3 wherein the filter has more than one cavity and the cavities are mounted relative to one another in a coaxial configuration.

18. A filter as claimed in any one of claims 1, 2 or 3 wherein said first cavity resonates in three orthogonal modes substantially simultaneously.

19. A filter as claimed in any one of claims 1, 2 or 3 wherein said first cavity resonates in three orthogonal modes substantially simultaneously, said first cavity containing three amounts of dielectric material, one amount to primarily affect each mode.

20. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric material has a dielectric constant greater than 30.

21. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric constant has a temperature coefficient greater than -200 ppm/°

C.

22. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric material has a Q greater than 1000.

23. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric material has a dielectric constant greater than 80.

24. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric constant has a temperature coefficient greater than -400 ppm/°

C.

25. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric material has a Q greater than 4000.

26. A filter as claimed in any one of claims 1, 2 or 3 wherein the material from which the cavity is made is selected from the group of Invar, titanium, aluminum graphite composite, metal composite and aluminum alloy.

27. A filter as claimed in any one of claims 1, 2 or 3 wherein material from which the cavity is constructed is selected from the group of aluminum silicon, aluminum beryllium and aluminum silicon carbide.

28. A filter as claimed in any one of claims 1, 2 or 3 wherein a temperature stability of the filter does not exceed 1 ppm/°

C.

29. A filter as claimed in any one of claims 1, 2 or 3 wherein a temperature stability of the filter does not exceed 1/2 ppm/°

C.

30. A filter as claimed in any one of claims 1, 2 or 3 wherein the filter has more than one cavity and a temperature stability of the filter does not exceed 1 ppm/°

C.

31. A filter as claimed in any one of claims 1, 2 or 3 wherein the filter has more than one cavity and a temperature stability of the filter does not exceed 1/2 ppm/°

C.

32. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric material is made of a titanium oxide base material.

45. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric constant has a temperature coefficient greater than +200 ppm/°

C.

46. A filter as claimed in any one of claims 1, 2 or 3 wherein said dielectric constant has a temperature coefficient greater than +400 ppm/°

C.

33. A method of constructing and compensating a microwave filter having a first cavity resonating at an operating frequency in at least two orthogonal modes substantially simultaneously, said cavity being made of a material having a coefficient of thermal expansion and having a volume that changes with temperature, said method comprising the steps of selecting one amount and type of dielectric material to be contained within said cavity for each mode, selecting the amount of dielectric material so that the dielectric material does not resonate at the operating frequency of the cavity, selecting the dielectric material with a dielectric constant and a temperature coefficient for the dielectric constant to compensate for changes in the volume in the cavity with temperature to at least reduce a variation in said operating frequency that would otherwise be caused by a temperature-induced volume change of said cavity.

34. A method as claimed in claim 33 including the steps of selecting the location of the dielectric material in the cavity for each mode.

35. A method as claimed in claim 34 including the steps of selecting the dielectric constant and the temperature coefficient of the dielectric constant for the dielectric material so that a variation in operating frequency that would otherwise result from any increase or decrease in temperature due to a change in volume of the cavity is approximately balanced by the variation in operating frequency that results from the change in the dielectric constant with temperature, thereby maintaining the operating frequency of the cavity substantially constant with temperature.

36. A method as claimed in any one of claims 33, 34 or 35 wherein the amount of dielectric material contained within the cavity is adjustable externally, said method including the steps of constructing the filter and operating the filter with a first fixed amount of dielectric material in said cavity for each mode, varying the temperature of the cavity and determining the temperature stability of the filter based on any change in the operating frequency in the filter with temperature, deciding whether the temperature stability of the filter is at an acceptable level, if said temperature stability of said filter is not at an acceptable level, varying the amount of dielectric material in said cavity for each mode to a second fixed amount and operating the filter while varying the temperature of the cavity, determining the temperature stability of said filter and repeating the steps of varying the amount of dielectric material contained in the cavity for each mode and operating the filter at varying temperatures until the temperature stability of the filter is at an acceptable level.

37. A method as claimed in any one of claims 33, 34 or 35 wherein said amount of dielectric material contained within the cavity is adjustable externally, said method including the steps of determining each amount of dielectric material within each cavity to ensure that an amount of dielectric material within a first cavity for a first mode is exactly the same as the amount of dielectric material within the cavity for a second mode, each cavity having two ends, said steps using means to measure a frequency of resonance peaks from reflection for each mode, said steps including simultaneously exciting said first cavity with a first mode from one end and a second mode from an opposite end, said modes being rotated 90°

from one another, determining the frequency of the resonance peak for each mode, adjusting at least one of the dielectric screws until a frequency of the resonance peaks are identical for the first and second modes.

38. A method as claimed in any one of claims 33, 34 or 35 wherein said method includes the steps of selecting a dielectric material having a dielectric constant greater than thirty.

39. A method as claimed in any one of claims 33, 34 or 35 wherein said method includes the steps of selecting a dielectric material having a temperature coefficient of the dielectric constant greater than -200 ppm/°

C.

40. A method as claimed in any one of claims 33, 34 or 35 wherein the method includes the steps of selecting a dielectric material having a Q greater than 1000.

41. A method as claimed in any one of claims 33, 34 or 35 wherein said method includes the steps of selecting a dielectric material having a dielectric constant greater than 80.

42. A method as claimed in any one of claims 33, 34 or 35 wherein said method includes the steps of selecting a dielectric material having a temperature coefficient of the dielectric constant greater than -400 ppm/°

C.

43. A method as claimed in any one of claims 33, 34 or 35 wherein said method includes the steps of selecting a dielectric material having a Q greater than 4000.

44. A method as claimed in any one of claims 33 or 34 wherein said method includes the step of selecting the dielectric material with a dielectric constant to compensate for changes in volume in the cavity with temperature to minimize a variation in said operating frequency that would otherwise be caused by a temperature-induced volume change of said cavity.

47. A method as claimed in any one of claims 33, 34 or 35 wherein said method includes the steps of selecting a dielectric material having a temperature coefficient of the dielectric constant greater than +200 ppm/°

C.

48. A method as claimed in any one of claims 33, 34 or 35 wherein said method includes the steps of selecting a dielectric material having a temperature coefficient of the dielectric constant greater than +400 ppm/°

C.